JPS6021301A - Iron powder for compacted magnetic core - Google Patents

Iron powder for compacted magnetic core

Info

Publication number
JPS6021301A
JPS6021301A JP58126478A JP12647883A JPS6021301A JP S6021301 A JPS6021301 A JP S6021301A JP 58126478 A JP58126478 A JP 58126478A JP 12647883 A JP12647883 A JP 12647883A JP S6021301 A JPS6021301 A JP S6021301A
Authority
JP
Japan
Prior art keywords
iron powder
powder
magnetic
magnetic core
apparent density
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP58126478A
Other languages
Japanese (ja)
Inventor
Shigeaki Takagi
高城 重彰
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
JFE Steel Corp
Original Assignee
Kawasaki Steel Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Kawasaki Steel Corp filed Critical Kawasaki Steel Corp
Priority to JP58126478A priority Critical patent/JPS6021301A/en
Publication of JPS6021301A publication Critical patent/JPS6021301A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain iron powder having a specified grain size and a specified density and giving magnetic core with high DC magnetic permeability and superior frequency characteristics by reducing iron oxide. CONSTITUTION:This iron powder for a compacted magnetic core has 50-270mum average grain size measured by sieve analysis and 2.8-3.5g/cm<2> apparent density, and it is manufactured by reducing iron oxide. The iron powder is compacted and hardened with resin or the like to form a starting material for a compacted magnetic core used as a reactor core, a noise filter core or the like. When the starting material is used, a compacted magnetic core with superior magnetic characteristics, especially frequency characteristics can be obtd. stably.

Description

【発明の詳細な説明】 この発明は、リアクトル・コアやノイズフィルター・コ
アなどに用いられる圧粉磁心の原料となる鉄粉に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to iron powder that is a raw material for powder magnetic cores used in reactor cores, noise filter cores, and the like.

周知のように鉄粉を圧粉成形して、樹脂などで固めた圧
粉磁心は、通常の全屈磁性材料にくらべて周波数特性が
良好であり、またフェライトにくらべて温度安定性が優
れ、飽和磁束密度が高く、印加磁界に対する透磁率の変
動が小さく、更には低価格で製造できるなどの利点を有
し、そのためリアクトル・コアやノイズフィルター°コ
アなどに利用されている。
As is well known, a powder magnetic core made by compacting iron powder and solidifying it with resin etc. has better frequency characteristics than normal totally magnetotropic materials, and has better temperature stability than ferrite. It has the advantages of high saturation magnetic flux density, small fluctuations in magnetic permeability with respect to applied magnetic field, and can be manufactured at low cost, so it is used for reactor cores, noise filter cores, etc.

どころで圧粉磁心の重要な特性としは、直流磁界に対す
る透磁率(直流透磁率)が大きいことと、周波数特性が
良好であることが上げられる。これらのうち、第一の点
、すなわち直流透磁率は、圧粉磁心の密度と密接な関係
があり、高い圧力で成形するか、あるいは純度の高い圧
縮性の良好な鉄粉を使用することによって、比較的筒単
に向上させることができる。しかしながら第二の点、す
なわち周波数特性に対しては、これに及はづ一鉄粉性状
の影響が充分に解明されていないため、従来は他の用途
に用いられている通常の粉末冶金用鉄粉をそのまま圧粉
磁心に流用しているのが実情であり、そのため従来の圧
粉磁心においては必ずしもその周波数特性が満足できる
程度まで達しないことも多いのが実情であった。
By the way, the important properties of a powder magnetic core include high magnetic permeability to a DC magnetic field (DC magnetic permeability) and good frequency characteristics. Among these, the first point, DC magnetic permeability, is closely related to the density of the powder magnetic core, and can be achieved by compacting at high pressure or using iron powder with high purity and good compressibility. , it can be improved relatively simply. However, regarding the second point, that is, the influence of iron powder properties on frequency characteristics, which has not been fully elucidated, The reality is that powder is used as is in powder magnetic cores, and as a result, the frequency characteristics of conventional powder magnetic cores often do not always reach a satisfactory level.

この発明は以上の事情に鑑みてなされたもので、圧粉磁
心の周波数特性と鉄粉性状との関係についての本発朗者
等の新規な知見に基づき、良好な周波数特性を安定して
得るための、通常の粉末冶金用鉄粉とは異なる鉄粉を提
供することを目的とするものである。
This invention has been made in view of the above circumstances, and is based on the novel knowledge of the present author and others regarding the relationship between the frequency characteristics of a powder magnetic core and the properties of iron powder, to stably obtain good frequency characteristics. The purpose of this invention is to provide an iron powder different from ordinary iron powder for powder metallurgy.

次にこの発明の基礎となった本発明者等の知見について
説明する。
Next, the findings of the present inventors, which formed the basis of this invention, will be explained.

圧粉磁心は、一般の磁性材料と同様に、使用周波数が高
くなるに従って透Pi率が直流透磁率に対し低下し、同
時に損失が増大して、ついには磁性材料として使用不可
能となる。圧粉磁心の場合、このような周波数特性に大
きく影響を及ぼすのは、本発明者等の見解によれば、(
1)粒子間の絶縁状態および(2)粒子の粒度であると
考えられる。
As with general magnetic materials, as the operating frequency increases, the powder magnetic core's Pi permeability decreases relative to its DC permeability, and at the same time its loss increases, eventually making it unusable as a magnetic material. In the case of powder magnetic cores, it is the opinion of the present inventors that (
It is thought that 1) the insulation state between particles and (2) the particle size of the particles.

すなわち(1)については、鉄粉粒子が互いに圧着して
絶縁が劣化すると、圧粉磁心の見掛の電気抵抗が低下し
て、交流磁界を印加した際に粒子間に渦電流が流れやす
くなり、磁気特性が劣化する。
In other words, regarding (1), when the iron powder particles are pressed together and the insulation deteriorates, the apparent electrical resistance of the powder magnetic core decreases, making it easier for eddy currents to flow between the particles when an alternating magnetic field is applied. , the magnetic properties deteriorate.

一方(2)については、粒子間の絶縁が充分であっても
、鉄粉粒子が粗大であれば、粒子内部に渦電流が流れや
すくなり、磁気特性が劣化する。
On the other hand, regarding (2), even if the insulation between the particles is sufficient, if the iron powder particles are coarse, eddy currents tend to flow inside the particles and the magnetic properties deteriorate.

したがって(2)の観点からは、良好な周波数特性を維
持するために、鉄粉粒子はあまり粗大でないことが望ま
れる。しかしながら逆にあまりに細かいと、鉄粉の圧縮
性が極端に劣化し、結果として直流透磁率が低下してし
まう。したがって狼粉粒子の粒度の下限と上限を規定す
べきであると考えられる。
Therefore, from the viewpoint of (2), in order to maintain good frequency characteristics, it is desirable that the iron powder particles are not too coarse. However, if the iron powder is too fine, the compressibility of the iron powder will be extremely degraded, resulting in a decrease in DC permeability. Therefore, it is considered that the lower and upper limits of the particle size of the powder powder should be defined.

一方(1)の観点からは、鉄粉の見掛密度は高いことが
望ましい。すなわち、見掛密度の低い鉄粉はど、粒子が
不規則な形状をしており、そのため圧粉成形した際に粒
子間の接触面積が大きく、粒子間の絶縁が劣化しやすい
からである。ところが逆に見掛密度があまりに高いと、
周知のように圧粉成形体の強度が低下し、樹脂などを用
いて固める場合においても、成形直後の取り扱いに余程
注意しなければ成形体を破壊するおそれがあり、好まし
くない゛。したがって鉄粉の見掛密度についても、その
下限と上限を規定すべきと考えられる。
On the other hand, from the viewpoint of (1), it is desirable that the apparent density of the iron powder is high. That is, iron powder with a low apparent density has irregularly shaped particles, and therefore, when compacted, the contact area between the particles is large, and the insulation between the particles is likely to deteriorate. However, if the apparent density is too high,
As is well known, the strength of the powder molded product decreases, and even if it is hardened using a resin or the like, there is a risk that the molded product will be destroyed if it is not handled with great care immediately after molding, which is not preferable. Therefore, it is considered that lower and upper limits should be specified for the apparent density of iron powder.

また以上のような考察からすれば、周波数特性の観点か
らは、鉄酸化物の還元によって製造される還元鉄粉より
も、溶鉄を水などで噴霧して製造されるアトマイズ鉄粉
の方が優れているよ、うに思ねれる。なぜならば、還元
鉄粉の見掛密度が通常2.5 g/cm程度であるのに
対しアトマイズ鉄粉の見掛密度は通常3.0 g/cm
’程度と、アトマイズ鉄粉の方が還元鉄粉よりも見掛密
度が高いからである。しかしながら本発明者等の詳細な
実験によれば、実際には還元鉄粉の方がアトマイズ鉄粉
よりも周波数特性が優れていることが判明した。この点
についてはのちに実験結果を用いて示すが、その理由は
次のように考えられる。すなわち、ふるい分析による粒
度が同程度であっても、還元鉄粉の粒子はその製造方法
に起因してスポンジ状となっているため、粒子内に空孔
の少ないアトマイズ鉄粉と比較して実質的には粒度が小
さいかのような効果を有するから、粒子内に渦電流が流
れにくく、良好な周波数特性が得られるのである。
In addition, from the above considerations, from the perspective of frequency characteristics, atomized iron powder produced by spraying molten iron with water is superior to reduced iron powder produced by reducing iron oxide. It seems like it is. This is because the apparent density of reduced iron powder is usually around 2.5 g/cm, whereas the apparent density of atomized iron powder is usually 3.0 g/cm.
This is because atomized iron powder has a higher apparent density than reduced iron powder. However, detailed experiments conducted by the present inventors have revealed that reduced iron powder actually has better frequency characteristics than atomized iron powder. This point will be shown later using experimental results, and the reason is thought to be as follows. In other words, even if the particle size according to sieve analysis is similar, reduced iron powder particles are spongy due to the manufacturing method, so compared to atomized iron powder, which has fewer pores within the particles, the reduced iron powder particles are actually smaller. In other words, since it has the effect of having a small particle size, it is difficult for eddy currents to flow within the particles, and good frequency characteristics can be obtained.

以上のように、優れた磁気特性を有する圧粉磁心を17
るためには、使用する鉄粉の粒度、見掛密度、および鉄
粉の製造方法に起因する鉄粉性状に着目しなければなら
ないにもかかわらず、従来はそれらの影響が充分に解明
されていなか1うたため、通常の粉末冶金用鉄粉が圧粉
磁心に使用されており、そのため充分な磁気特性が達成
されていなかったのである。
As mentioned above, 17 powder magnetic cores with excellent magnetic properties
In order to achieve this goal, it is necessary to focus on the particle size and apparent density of the iron powder used, as well as the iron powder properties caused by the iron powder manufacturing method. For one reason, ordinary iron powder for powder metallurgy was used in powder magnetic cores, and as a result, sufficient magnetic properties were not achieved.

そこで本発明者等は、前述した知見に基づき、規定すべ
き鉄粉粒子の粒度および見掛密度の範囲について詳輝に
実験を進めた結果、ふるい分析からめた平均粒径が50
〜210戸、見掛密度が2.8〜3.5 o/cmの範
囲内にある還元鉄粉が、圧粉磁心用鉄粉として優れてい
ることを見出し、この発明をなすに至ったのである。
Based on the above-mentioned knowledge, the present inventors carried out detailed experiments on the particle size and apparent density range of iron powder particles that should be specified, and as a result, the average particle size determined from sieve analysis was 50.
We discovered that reduced iron powder with an apparent density in the range of 2.8 to 3.5 o/cm is excellent as an iron powder for powder magnetic cores, and we came up with this invention. be.

したがってこの発明の圧粉磁心用鉄粉は、鉄酸化物の還
元によって製造される鉄粉であって、しかもふるい分析
によってめられる平均粒径が50〜270戸の範囲内に
あり、かつ見掛密度が2.8〜3.5 Q/G〆の範囲
内にあることを特徴とするものである。
Therefore, the iron powder for powder magnetic cores of the present invention is iron powder produced by reduction of iron oxide, has an average particle size determined by sieve analysis in the range of 50 to 270 particles, and has an apparent It is characterized by having a density within the range of 2.8 to 3.5 Q/G.

以下この発明を更に詳甲に説明する。This invention will be explained in more detail below.

先ず、ふるい分析による。平均粒径の上限を270声と
定めた理由について説明する。第1図は、見掛密度が3
.0±0.1g/C7とほぼ等しく、平均粒径の異なる
還元鉄粉および水アトマイズ鉄粉を用いて、それぞれ2
 t/ctの加圧力で圧粉成形して外径38’mm、内
径25IIl1111高さ6.5InIIlのリング状
成形体を作成し、インピーダンスメーターを用いて透磁
率の周波数依存性を測定することにより、限界周波数を
めた結果を示す。ここで限界周波数とは、便宜的に透磁
率が直流透磁率の80%となる周波数と定義している。
First, by sieve analysis. The reason why the upper limit of the average particle diameter was set at 270 tones will be explained. Figure 1 shows that the apparent density is 3
.. Using reduced iron powder and water atomized iron powder, which are approximately equal to 0 ± 0.1 g/C7 and have different average particle sizes,
A ring-shaped molded body with an outer diameter of 38'mm, an inner diameter of 25mm, and a height of 6.5mm was created by compacting with a pressure of t/ct, and the frequency dependence of magnetic permeability was measured using an impedance meter. , shows the result of finding the limit frequency. Here, the limit frequency is conveniently defined as the frequency at which the magnetic permeability becomes 80% of the DC magnetic permeability.

第10から明らかなように、平均粒径の小さいものはい
ずれの鉄粉でも限界周波数が0.3Ml−1z程度とな
っているが、還元鉄粉の場合、平均粒径が270声を越
えれば限界周波数が0.2MH2以下と小さくなり、良
好な周波数特性が要求される圧粉磁心には適さなくなる
As is clear from No. 10, any iron powder with a small average particle size has a critical frequency of about 0.3 Ml-1z, but in the case of reduced iron powder, if the average particle size exceeds 270 tones, The limit frequency is as small as 0.2 MH2 or less, making it unsuitable for powder magnetic cores that require good frequency characteristics.

したがつT 還元鉄粉の平均粒径の上限を270陣と定
めた。また第1図から、アトマイズ鉄粉は還元鉄粉より
も周波数特性が劣り、そのため良好な周波数特性が要求
される用途には適さないことが明らかである。
Therefore, the upper limit of the average particle size of reduced iron powder was set at 270 grains. Furthermore, from FIG. 1, it is clear that atomized iron powder has inferior frequency characteristics to reduced iron powder, and is therefore not suitable for applications requiring good frequency characteristics.

、次に、平均な径の下限を50JJI11とした根拠に
ついて説明す□る。第2図は第1図の測定で用いたと同
じ還元鉄粉による成形体の直流透磁率を測定した結果を
示す。第2図から、通常圧粉磁心に要求される透磁率の
最低値とされる40程度を確保するためには、平均粒径
を50pm以上としなければならないことが明らかであ
る。
Next, the basis for setting the lower limit of the average diameter to 50JJI11 will be explained. FIG. 2 shows the results of measuring the DC magnetic permeability of a molded body made of the same reduced iron powder used in the measurement of FIG. 1. From FIG. 2, it is clear that the average particle size must be 50 pm or more in order to secure the minimum magnetic permeability of about 40 normally required for powder magnetic cores.

一方、見掛密度の下限を2.8 MOIfiと定めたの
は次の理由による。第3図は、平均粒径がほぼ等しく、
見I!)密度の異なるミルスケール還元鉄粉を前記同様
にリング状に圧粉成形し、限界周波数をめた結果を示す
。第3図から、限界周波数0.2MHz以上を確保する
ためには、見掛密度が2.8g/cm以上でなければな
らないことが明らかである。
On the other hand, the reason why the lower limit of the apparent density was set at 2.8 MOIfi is as follows. Figure 3 shows that the average particle size is almost equal,
Look I! ) Mill-scale reduced iron powders with different densities were compacted into a ring shape in the same manner as above, and the results of determining the critical frequency are shown. From FIG. 3, it is clear that in order to ensure a critical frequency of 0.2 MHz or higher, the apparent density must be 2.8 g/cm or higher.

さらに、見掛密度の上限を3.5 a/cイと定めた理
由を第4図について説明する。この第4図は、第3図の
測定で用いたと同じ還元鉄粉を使用し、潤滑剤としてス
テアリン酸亜鉛を1重量%添加して5 t/c♂の加圧
力で圧粉成形し、長さ35PIII+、幅10III1
11高さ6FllI+の成形体を作成して、その抗折力
を測定した結果を示すものであり、見掛密度が3.5Q
/fJ’を越えれば、成形体として通常必要とされる抗
折ノ) 0.’5k(1/−が達成されないことが明ら
かである。したがって見掛密度は3.5 g/co1g
、下に収める必要がある。
Furthermore, the reason why the upper limit of the apparent density was set at 3.5 a/c will be explained with reference to FIG. This figure 4 shows that the same reduced iron powder used in the measurement in figure 3 was used, 1% by weight of zinc stearate was added as a lubricant, and the powder was compacted at a pressure of 5 t/c♂. Size 35PIII+, width 10III1
11 This shows the results of creating a molded body with a height of 6FllI+ and measuring its transverse rupture strength, and the apparent density is 3.5Q.
/fJ', the bending resistance normally required for a molded product is 0. '5k (1/- is clearly not achieved. Therefore, the apparent density is 3.5 g/co1g
, it needs to fit below.

以上のように原料鉄粉として、ミルスケール還元鉄粉な
どの還元鉄粉であってしかもその平均粒径が50〜27
0声、見掛密度が2.8〜3.5 g/amの範囲内の
鉄粉を使用することによって、はじめて優れた特性を有
する圧粉磁心が安定して得られることが明らかである。
As mentioned above, the raw material iron powder is reduced iron powder such as mill scale reduced iron powder and has an average particle size of 50 to 27
It is clear that a powder magnetic core having excellent properties can be stably obtained only by using iron powder having an apparent density of 2.8 to 3.5 g/am.

以下にこの発明の実施例を記す。Examples of this invention are described below.

実施例1 平均粒径78戸、見掛密度2.93(II/ cmのミ
ルスケール3■元鉄粉を2t/ c/で圧粉成形し、外
径38mm、内径25.mm、高さ6.5+!lII+
のリング状成形体を作成し、インピ−ダンスメーターに
より透磁率の周波数依存性を測定した結果、直流透m率
51、限界周波数0.29MH7を達成した。
Example 1 Mill scale 3 original iron powder with an average particle diameter of 78 mm and an apparent density of 2.93 (II/cm) was compacted at 2 t/c/, and had an outer diameter of 38 mm, an inner diameter of 25 mm, and a height of 6 mm. .5+!lII+
A ring-shaped molded body was prepared, and the frequency dependence of magnetic permeability was measured using an impedance meter. As a result, a DC permeability of 51 and a limit frequency of 0.29 MH7 were achieved.

実施例2 平均粒径215声、見掛密度3.03(J/C♂のミル
スケール還元鉄粉について、実施例1と同様な実験を行
ない、直流透磁率57、限界周波数0.28MH2を達
成した。
Example 2 An experiment similar to Example 1 was conducted using mill scale reduced iron powder with an average particle size of 215 mm and an apparent density of 3.03 (J/C♂), and a DC permeability of 57 and a limit frequency of 0.28 MH2 were achieved. did.

実施例3 平均粒径83pHl、見掛密痕3.22g/cイのミル
スケール還元鉄粉について、実施例1と同様な実験を行
ない、直流透磁率49、限界周波数0.38MH2を達
成した。
Example 3 An experiment similar to Example 1 was conducted using mill scale reduced iron powder with an average particle size of 83 pHl and an apparent density of 3.22 g/c, and a DC permeability of 49 and a limit frequency of 0.38 MH2 were achieved.

以上の説明で明らかなように、この発明の圧粉磁心用鉄
粉は、リアクトル・コアやノイズフィルター・コアなど
に用いられる圧粉磁心の原料粉末に最適なものであり、
これを用いることによって磁心としての磁気特性、特に
周波数特性の優れた圧粉磁心を安定して得ることができ
る。
As is clear from the above explanation, the iron powder for powder magnetic cores of the present invention is optimal as a raw material powder for powder magnetic cores used for reactor cores, noise filter cores, etc.
By using this, it is possible to stably obtain a powder magnetic core with excellent magnetic properties, especially frequency properties.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は還元鉄粉およびアトマイズ鉄粉の平均粒径とそ
れらの鉄粉を用いた成形体の限界周波数との関係を示す
相関図、第2図は還元鉄粉の平均粒径とそれを用いた鉄
粉成形体の直流透磁率との関係を示す相関図、第3図は
還元鉄′粉の見掛密度とそれを用いた鉄粉成形体の限稈
周波数との関係を示す相関図、第4図は還元鉄粉の見掛
密度とそれを用いた鉄粉成形体の抗折カとの関係を示す
相関図である。 出願人 川崎製鉄株式会社 代理人 弁理士 豊1)武久 (ばか1名) 第1区 平均粒怪(μm) 第2図 渠均救怪(、pun) 第3図 ″′( 椰 契L411ト〜p 度 ζμヨうン
Figure 1 is a correlation diagram showing the relationship between the average particle diameter of reduced iron powder and atomized iron powder and the critical frequency of a molded product using those iron powders, and Figure 2 is a correlation diagram showing the relationship between the average particle diameter of reduced iron powder and the limit frequency of a molded product using those iron powders. Figure 3 is a correlation diagram showing the relationship between the DC permeability of the iron powder compact used, and Figure 3 is a correlation diagram showing the relationship between the apparent density of reduced iron powder and the limiting frequency of the iron powder compact using it. , FIG. 4 is a correlation diagram showing the relationship between the apparent density of reduced iron powder and the bending force of an iron powder molded article using the same. Applicant Kawasaki Steel Co., Ltd. agent Patent attorney Yutaka 1) Takehisa (1 idiot) 1st ward average grain size (μm) Figure 2 Hitoshi Hitoshi (,pun) Figure 3''' ( Coconut L411 to ~ p degree ζμyoung

Claims (1)

【特許請求の範囲】[Claims] 鉄酸化物の還元によって製造される鉄粉であって、しか
もふるい分析によってめられる平均粒径が50〜270
声の範囲内にあり、かつ見掛密度が2.8〜3.5 M
C♂の範囲内にあることを特徴とする圧ね磁心用鉄粉。
Iron powder produced by reduction of iron oxide, with an average particle size of 50 to 270 as determined by sieve analysis.
Within the voice range and with an apparent density of 2.8 to 3.5 M
An iron powder for pressurized magnetic cores characterized by being within the range of C♂.
JP58126478A 1983-07-11 1983-07-11 Iron powder for compacted magnetic core Pending JPS6021301A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58126478A JPS6021301A (en) 1983-07-11 1983-07-11 Iron powder for compacted magnetic core

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58126478A JPS6021301A (en) 1983-07-11 1983-07-11 Iron powder for compacted magnetic core

Publications (1)

Publication Number Publication Date
JPS6021301A true JPS6021301A (en) 1985-02-02

Family

ID=14936208

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58126478A Pending JPS6021301A (en) 1983-07-11 1983-07-11 Iron powder for compacted magnetic core

Country Status (1)

Country Link
JP (1) JPS6021301A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62222002A (en) * 1986-03-20 1987-09-30 Hitachi Metals Ltd Production of dust core of fe-si-al alloy
JPS62250607A (en) * 1986-04-23 1987-10-31 Hitachi Metals Ltd Manufacture of fe-si-al alloy dust core

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62222002A (en) * 1986-03-20 1987-09-30 Hitachi Metals Ltd Production of dust core of fe-si-al alloy
JPH0348241B2 (en) * 1986-03-20 1991-07-23 Hitachi Metals Ltd
JPS62250607A (en) * 1986-04-23 1987-10-31 Hitachi Metals Ltd Manufacture of fe-si-al alloy dust core

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